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21—30 of 616 matching pages
21: 14.33 Tables
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Abramowitz and Stegun (1964, Chapter 8) tabulates for , , 5–8D; for , , 5–7D; and for , , 6–8D; and for , , 6S; and for , , 6S. (Here primes denote derivatives with respect to .)
Zhang and Jin (1996, Chapter 4) tabulates for , , 7D; for , , 8D; for , , 8S; for , , 8D; for , , , , 8S; for , , 8S; for , , , 5D; for , , 7S; for , , 8S. Corresponding values of the derivative of each function are also included, as are 6D values of the first 5 -zeros of and of its derivative for , .
Belousov (1962) tabulates (normalized) for , , , 6D.
22: 26.7 Set Partitions: Bell Numbers
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is the number of partitions of .
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26.7.1
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26.7.2
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26.7.6
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►For higher approximations to as see de Bruijn (1961, pp. 104–108).
23: 18.8 Differential Equations
24: Bibliography D
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The principal frequencies of vibrating systems with elliptic boundaries.
Quart. J. Mech. Appl. Math. 8 (3), pp. 361–372.
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Handbuch der Laplace-Transformation. Bd. II. Anwendungen der Laplace-Transformation. 1. Abteilung.
Birkhäuser Verlag, Basel und Stuttgart (German).
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Inequalities for extreme zeros of some classical orthogonal and -orthogonal polynomials.
Math. Model. Nat. Phenom. 8 (1), pp. 48–59.
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Lamé instantons.
J. High Energy Phys. 2000 (1), pp. Paper 19, 8.
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Product formulas and Nicholson-type integrals for Jacobi functions. I. Summary of results.
SIAM J. Math. Anal. 9 (1), pp. 76–86.
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25: 3.5 Quadrature
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►If in addition is periodic, , and the integral is taken over a period, then
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►If , then the remainder in (3.5.2) can be expanded in the form
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►For the Bernoulli numbers see §24.2(i).
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►For further information, see Mason and Handscomb (2003, Chapter 8), Davis and Rabinowitz (1984, pp. 74–92), and Clenshaw and Curtis (1960).
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►For functions Gauss quadrature can be very efficient.
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26: 26.13 Permutations: Cycle Notation
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26.13.2
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…In consequence, (26.13.2) can also be written as .
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►For the example (26.13.2), this decomposition is given by
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►Again, for the example (26.13.2) a minimal decomposition into adjacent transpositions is given by : .
27: 12.14 The Function
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►For the modulus functions and see §12.14(x).
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►Other expansions, involving and , can be obtained from (12.4.3) to (12.4.6) by replacing by and by ; see Miller (1955, p. 80), and also (12.14.15) and (12.14.16).
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►uniformly for , with , , , and as in §12.10(vii).
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or is the modulus and or is the corresponding phase.
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►For properties of the modulus and phase functions, including differential equations and asymptotic expansions for large , see Miller (1955, pp. 87–88).
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28: 2.10 Sums and Sequences
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►For further information on see §5.17.
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►For extensions to , higher terms, and other examples, see Olver (1997b, Chapter 8).
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►For generalizations and other examples see Olver (1997b, Chapter 8), Ford (1960), and Berndt and Evans (1984).
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►For examples see Olver (1997b, Chapters 8, 9).
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►For other examples and extensions see Olver (1997b, Chapter 8), Olver (1970), Wong (1989, Chapter 2), and Wong and Wyman (1974).
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29: 1.11 Zeros of Polynomials
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►Set to reduce to , with , .
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, , , .
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►Resolvent cubic is with roots , , , and , , .
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►Let
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►Then , with , is stable iff ; , ; , .
30: Bibliography L
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On the maxima and minima of Bernoulli polynomials.
Amer. Math. Monthly 47 (8), pp. 533–538.
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A partition function connected with the modulus five.
Duke Math. J. 8 (4), pp. 631–655.
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On the theory of diffraction by an aperture in an infinite plane screen. I.
Phys. Rev. 74 (8), pp. 958–974.
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Monotonicity and convexity properties of zeros of Bessel functions.
SIAM J. Math. Anal. 8 (1), pp. 171–178.
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Solutions of the fifth Painlevé equation.
Differ. Uravn. 4 (8), pp. 1413–1420 (Russian).
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